Step 1: Understand the concept
The charge gains kinetic energy equal to the work done by the field. Later, at the closest approach, all that kinetic energy has become electrostatic potential energy.
Step 2: Energy gained
The force is \(qE\) over a distance \(D\), so the kinetic energy gained is \(K = qED\).
Step 3: Energy at closest approach
At the closest distance \(r\) the speed is zero, so \(K = \dfrac{qQ}{4\pi\varepsilon_0 r}\) (the starting potential energy at large distance is zero).
Step 4: Solve
\[ qED = \frac{qQ}{4\pi\varepsilon_0 r} \Rightarrow r = \frac{Q}{4\pi\varepsilon_0ED} \]
Option (B). The charge \(q\) and the mass \(m\) cancel out.
Final Answer:
The closest approach is Q/(4 pi epsilon_0 E D). This is option (B).
\[ \boxed{\text{(B) }\frac{Q}{4\pi\varepsilon_0ED}} \]